XL International Symposium on Multiparticle Dynamics Inclusive cross sections of proton-proton and proton-antiproton scattering Victor A. Abramovsky Natalia V. Radchenko Novgorod State University Russia

ISMD Inclusive cross sections and multiplicity distributions are different for pp and pbarp Pomeranchuk theorem: total cross sections differential elastic cross sections the same elastic cross sections for pp and pbarp It is also generally accepted that inclusive cross sections and multiplicity distributions are the same for pp and pbarp.

ISMD Low Constituents Number Model (LCNM) 1.On the first step before the collision there is small number of constituents in initial hadrons. In every hadron this is component either with only valence quarks or with valence quarks and one additional gluon. 2.On the second step the hadrons interaction is carried out by gluon exchange between the valence quarks and initial gluons. The hadrons gain the color charge. 3.On the third step after interaction the colored hadrons move apart and when the distance between them becomes larger than the confinement radius, the lines of color electric field gather into the string. This string breaks out into secondary hadrons. (Abramovsky, Kancheli 1980, Abramovsky, Radchenko 2009)

ISMD Three types of inelastic subprocesses

ISMD Results in LCNM

ISMD Pseudorapidity density at LHC energies

ISMD The importance of inclusive cross sections From the LCNM it follows, that multiplicity distributions are different for pp and pbarp because of subprocess with three quark strings in pbarp (blue line). Three quark strings produce events with high multiplicity in tail of distribution. In order to make the difference more visible, we have to use observable instead of is measured independently of in inclusive measurements

ISMD Inclusive cross sections in events with fixed number of particles Topological inclusive cross section of one charged particle production Total inclusive cross section and its normalization Normalization of topological inclusive cross section

ISMD Inclusive cross sections in bins UA5 Coll. gave data in 9 bins of charged multiplicities: 2 ≤ n ≤ 10, 12 ≤ n ≤ 20, … 72 ≤ n ≤ 80 and n ≥ 82. We define inclusive cross section in this bins Inclusive cross sections in bins are normalized as follows

ISMD Difference in inclusive cross sections of pp and pbarp Ratio of (1) to (2) gives Solution of the integral equation (3) (perhaps, the only solution)

ISMD Inclusive cross sections in different bins 2 ≤ n ≤ ± ≤ n ≤ ± ≤ n ≤ ± ≤ n ≤ ± ≤ n ≤ ± ≤ n ≤ ± ≤ n ≤ ± ≤ n ≤ ± 0.02 n ≥ ± 0.02

ISMD Inclusive cross sections summed over all bins We obtained the numerical value of relation by summing over all nine bins of multiplicity. For This result will be used on the next slides.

ISMD Inclusive cross section with transverse momentum From the AGK cancellation rules it follows the factorization of transverse dependence in inclusive cross section. Returning to formulas (1) and (2) we can write down From this relation it can strictly be proved that so we can obtain

ISMD Experimental evidences of difference in pp and pbarp ATLAS Coll. ALICE Coll.

ISMD Conclusion We think that ATLAS Coll. discovered a new effect – the difference in multiparticle production in pp and pbarp interactions. ALICE Coll. confirmed this effect. We propose to experimentalists to measure inclusive cross section in bins with high multiplicities, where the difference will be the most evident.

ISMD Acknowledgements V.A.A. gratefully acknowledges financial support from the RFBR, grant z. N.V.R. gratefully acknowledges financial support from the Ministry of education and science of the Russian Federation, grant P1200.